( 813 ) 
be the probabilities of two different 
line-ensemble 
wy rie 2 Ms 
Wo Py v, 
for the energy space-ensemble 
W,  %; 
w oF U 
1 
States, then we have for the 
(10); 
teks 
for the microcanonical and the time-ensemble 
Wy — Ww, 
We can represent the probability of 
C 
1 
for the line-ensemble, 
for the energy space-ensemble and 
Hs OF 
for the microcanonical ensemble *). 
(12). 
a given system by 
1) In order to determine the constants Cy and Cs we can proceed in the following 
way. The number of systems in an element dw of the energy space-ensemble and 
y 
in an element dp,...dqn of the microcanonical ensemble amounts to 2 de 
v 
and N! C; dp). dgn, if N and N! represent the tolal number of systems in the 
ensemble. It is easily shown now that we have 
Patel dw ie “dw 
eed =| de 
E / 2 
Ee ON 
where the integration has to be extended over the space H2,—;. And further 
~ dq, = 
~ a 1 
= [dos == de | eed 
v 
g E 
the integral_| has to be extended over the 
layer between E2n—1 and E'2n—1, 
and the integral again over the space Kan. 
BE 
In determining the constant C, we have to 
the first place if the path L is closed we find 
distinguish between two cases. In 
